Optical module for atomic oscillator and atomic oscillator

ABSTRACT

An optical module for an atomic oscillator using a quantum interference effect includes a light source adapted to emit light including a fundamental wave having a predetermined wavelength, and sideband waves of the fundamental wave, a wavelength selection section receiving the light from the light source, and adapted to transmit the sideband waves out of the light input, a gas cell encapsulating an alkali metal gas, and irradiated with light transmitted through the wavelength selection section, and a light detection section adapted to detect an intensity of light transmitted through the gas cell, and the wavelength selection section includes a fiber Bragg grating, and a temperature control section adapted to control temperature of the fiber Bragg grating.

BACKGROUND

1. Technical Field

The present invention relates to an optical module for an atomic oscillator and an atomic oscillator.

2. Related Art

In recent years, an atomic oscillator using coherent population trapping (CPT) as a quantum interference effects has been proposed, and downsizing of the device and reduction in power consumption have been expected. An atomic oscillator using CPT is an oscillator using a phenomenon (an electromagnetically induced transparency (EIT) phenomenon) that exists if an alkali metal atom is irradiated with two resonance lights with respective wavelengths (frequencies) that are different from each other at the same time. As a result, absorption of the two resonance lights stops. For example, in JP-A-2009-89116, there is described an atomic oscillator as an atomic oscillator using CPT, which is configured to include an optical module having a light source for emitting a coherent light, a gas cell for encapsulating alkali metal atoms, and a light receiving element for detecting the intensity of the light transmitted through the gas cell.

In the atomic oscillator using CPT, a semiconductor laser is used, for example, as the light source. In the atomic oscillator using the semiconductor laser as the light source, for example, the drive current of the semiconductor laser is modulated to thereby cause a sideband wave in the light emitted from the semiconductor laser, and thus the EIT phenomenon is developed.

However, the light emitted from the semiconductor laser the drive current of which is modulated includes not only the sideband wave but also a fundamental wave (a carrier wave) having a center wavelength making no contribution to the EIT phenomenon. If the alkali metal atoms are irradiated with the fundamental wave, there is a case in which the wavelength (the frequency) of the light absorbed by the alkali metal atoms varies (the AC Stark effect) to thereby degrade the stability of the frequency of the atomic oscillator.

SUMMARY

An advantage realized by some aspects of the invention is to provide an optical module for an atomic oscillator, which is capable of providing an atomic oscillator with high frequency stability. Further, another advantage realized by some aspects of the invention is to provide an atomic oscillator having the optical module for an atomic oscillator, described above.

An aspect of the invention is directed to an optical module for an atomic oscillator using a quantum interference effect including a light source adapted to emit light including a fundamental wave having a predetermined wavelength, and sideband waves of the fundamental wave, a wavelength selection section receiving the light from the light source, and adapted to transmit the sideband waves out of the light input, a gas cell encapsulating an alkali metal gas, and irradiated with light transmitted through the wavelength selection section, and a light detection section adapted to detect an intensity of light transmitted through the gas cell, wherein the wavelength selection section includes a fiber Bragg grating, and a temperature control section adapted to control temperature of the fiber Bragg grating.

According to such an optical module for an atomic oscillator, the wavelength selection section can decrease the intensity of the fundamental wave included in the light from the light source or eliminate the fundamental wave. Thus, it is possible to control or prevent the alkali metal atom from being irradiated with the fundamental wave making no contribution to the EIT phenomenon. Therefore, it is possible to reduce the frequency variation due to the AC Stark effect to thereby provide an oscillator with high frequency stability. Further, since the wavelength selection section has the temperature control section for controlling the temperature of the fiber Bragg grating, the wavelength selection characteristics (the wavelength range of the light to be selected by the fiber Bragg grating) of the fiber Bragg grating can be varied using the thermooptic effect. Thus, the wavelength selection section can correct the shift in the wavelength selection characteristics of the fiber Bragg grating due to manufacturing error, environmental variation, and so on.

The optical module for an atomic oscillator of the above aspect of the invention may be configured such that the temperature control section includes a resistive element presenting a predetermined resistance value, and controls the temperature of the fiber Bragg grating by controlling a current to be applied to the resistive element.

According to such an optical module for an atomic oscillator, the wavelength selection section can be made to have a simple configuration.

The optical module for an atomic oscillator of the above aspect of the invention may be configured such that the light source is a surface emitting laser.

According to such an optical module for an atomic oscillator, since the surface emitting laser requires a small current for generating the gain compared to the edge emitting laser, reduction in power consumption can be achieved.

The optical module for an atomic oscillator of the above aspect of the invention may be configured to further include an optical element adapted to make the light emitted from the light source enter the fiber Bragg grating.

According to such an optical module for an atomic oscillator, it is possible to efficiently guide the light emitted from the light source to the fiber Bragg grating.

Another aspect of the invention is directed to an atomic oscillator including the optical module for an atomic oscillator of the above aspect of the invention.

Since such an atomic oscillator includes the optical module for an atomic oscillator according to the aspect of the invention described above, it is possible to reduce the frequency variation due to the AC Stark effect to thereby enhance the frequency stability.

Still another aspect of the invention is directed to an atomic oscillator using a quantum interference effect including a light source adapted to emit light including a fundamental wave having a predetermined wavelength, and sideband waves of the fundamental wave, a wavelength selection section receiving the light from the light source, and adapted to transmit the sideband waves out of the light input, a gas cell encapsulating an alkali metal gas, and irradiated with light transmitted through the wavelength selection section, and a light detection section adapted to detect an intensity of light transmitted through the gas cell, wherein the wavelength selection section includes a fiber Bragg grating, and a temperature control section adapted to control temperature of the fiber Bragg grating.

According to such an atomic oscillator, the wavelength selection section can decrease the intensity of the fundamental wave included in the light from the light source or eliminate the fundamental wave. Thus, it is possible to control or prevent the alkali metal atom from being irradiated with the fundamental wave making no contribution to the EIT phenomenon. Therefore, it is possible to reduce the frequency variation due to the AC Stark effect to thereby provide an oscillator with high frequency stability. Further, since the wavelength selection section has the temperature control section for controlling the temperature of the fiber Bragg grating, the wavelength selection characteristics (the wavelength range of the light to be selected by the fiber Bragg grating) of the fiber Bragg grating can be varied using the thermooptic effect. Thus, the wavelength selection section can correct the shift in the wavelength selection characteristics of the fiber Bragg grating due to manufacturing error, environmental variation, and so on.

BRIEF DESCRIPTION OF THE DRAWINGS

The invention will be described with reference to the accompanying drawings, wherein like numbers reference like elements.

FIG. 1 is a functional block diagram of an atomic oscillator according to an embodiment of the invention.

FIG. 2A is a diagram showing a relationship between a Λ-type three-level model of an alkali metal atom, and a first sideband wave and a second sideband wave, and FIG. 2B is a diagram showing a frequency spectrum of a first light generated by the light source.

FIG. 3 is a diagram showing a frequency spectrum of a second light emitted from a wavelength selection section.

FIG. 4 is a block diagram showing a configuration of the atomic oscillator according to the present embodiment.

FIG. 5 is a perspective view schematically showing a substantial part of an optical module according to the present embodiment.

DESCRIPTION OF AN EXEMPLARY EMBODIMENT

An exemplary embodiment of the invention will hereinafter be described with reference to the accompanying drawings.

Firstly, an optical module and an atomic oscillator according to the embodiment will be explained with reference to the accompanying drawings. The atomic oscillator according to the present embodiment includes an optical module according to the present embodiment. FIG. 1 is a functional block diagram of the atomic oscillator 1 according to the present embodiment. The atomic oscillator 1 is an oscillator using a quantum interference effect.

The atomic oscillator 1 includes an optical module 2 and a control section 50.

The optical module 2 includes a light source 10, a wavelength selection section 20, a gas cell 30, and a light detection section 40.

The light source 10 generates a first light L1 including a fundamental wave F having a predetermined center wavelength (center frequency), and first and second sideband waves W1, W2 having respective wavelengths different from each other.

The wavelength selection section 20 selects the first and second sideband waves W1, W2 from the first light L1, and then emits it as a second light L2. The wavelength selection section 20 has a fiber Bragg grating (hereinafter also referred to an “FBG”) 20 a for selectively emitting light in a predetermined wavelength range, and a temperature control section 20 b for controlling the temperature of the FBG 20 a. The temperature control section 20 b can vary the wavelength range for the selection (wavelength selection characteristics) of the FBG 20 a by controlling the temperature of the FBG 20 a.

The gas cell 30 encapsulates an alkali metal gas, and is irradiated with the second light L2.

The light detection section 40 detects the intensity of the second light L2 transmitted through the gas cell 30.

The control section 50 performs control so that the difference in wavelength (frequency) between the first sideband wave W1 and the second sideband wave W2 becomes equal to the frequency corresponding to the difference in energy between the two ground levels of the alkali metal atoms encapsulated in the gas cell 30 based on the detection result of the light detection section 40. The control section 50 generates a detection signal having a modulation frequency f_(m) based on the detection result of the light detection section 40. Then, the light source 10 modulates the fundamental wave F having a predetermined frequency f₀ based on the detection signal to thereby generate the first sideband wave W1 having a frequency f₁=f₀+f_(m), and the second sideband wave W2 having a frequency f₂=f₀−f_(m).

FIG. 2A is a diagram showing a relationship between a Λ-type three-level model of the alkali metal atoms, and the first sideband wave W1 and the second sideband wave W2. FIG. 2B is a diagram showing a frequency spectrum of the first light L1 generated by the light source 10.

As shown in FIG. 2B, the first light L1 generated in the light source 10 includes the fundamental wave F having the center frequency f₀ (=ν/λ₀: ν denotes the speed of light; and λ₀ denotes the center wavelength of the laser beam), the first sideband wave W1 having the frequency f₁ in the upper sideband with respect to the center frequency f₀, and the second sideband wave W2 having the frequency f₂ in the lower sideband with respect to the center frequency f₀. The frequency f₁ of the first sideband wave W1 is obtained as f₁=f₀+f_(m), and the frequency f₂ of the second sideband wave W2 is obtained as f₂=f₀−f_(m).

As shown in FIGS. 2A and 2B, the frequency difference between the frequency f₁ of the first sideband wave W1 and the frequency f₂ of the second sideband wave W2 coincides with the frequency corresponding to the energy difference ΔE₁₂ between the ground level GL1 and the ground level GL2 of the alkali metal atom. Therefore, the alkali metal atoms cause the EIT phenomenon with the first sideband wave W1 having the frequency f₁ and the second sideband wave W2 having the frequency f₂.

Here, the EIT phenomenon will be explained. There is known that the interaction between an alkali metal atom and the light can be explained with the Λ-type three-level model. As shown in FIG. 2A, an alkali metal atom has two ground levels, and if the alkali metal atom is irradiated with either one of the first sideband wave W1 having the wavelength (frequency f₁) corresponding to the energy difference between the ground level GL1 and the excitation level and the second sideband wave W2 having the wavelength (frequency f₂) corresponding to the energy difference between the ground level GL2 and the excitation level alone, light absorption occurs. However, as shown in FIG. 2B, if an alkali metal atom is irradiated with the first sideband wave W1 and the second sideband wave W2 having the respective frequencies f₁, f₂ the difference of which (f₁−f₂) accurately coincides with the frequency corresponding to the energy difference ΔE₁₂ between the ground level GL1 and the ground level GL2 simultaneously, a superposition state of the two ground levels, namely the quantum interference state, occurs to thereby cause a transparency phenomenon (the EIT phenomenon) in which the excitation to the excitation level stops, and the first sideband wave W1 and the second sideband wave W2 are transmitted through the alkali metal atom. By detecting and then controlling the steep variation in the light absorption behavior occurring when the frequency difference f₁−f₂ between the first sideband wave W1 and the second sideband wave W2 is shifted from the frequency corresponding to the energy difference ΔE₁₂ between the ground level GL1 and the ground level GL2 using the EIT phenomenon, a highly accurate oscillator can be manufactured.

However, if the gas cell 30 is directly irradiated with the first light L1 shown in FIG. 2B, the gas cell, namely the alkali metal atoms, is irradiated with the fundamental wave F simultaneously with the first sideband wave W1 and the second sideband wave W2. If the alkali metal atoms are irradiated with the fundamental wave F making no contribution to the EIT phenomenon, the wavelength (frequency) of the light absorbed by each the alkali metal atom varies due to the AC Stark effect. Thus, the amount of the first sideband wave W1 and the second sideband wave W2 transmitted through the alkali metal atoms varies. In the oscillator using the EIT phenomenon, the amount of the first sideband wave W1 and the second sideband wave W2 transmitted through the alkali metal atoms is detected to thereby stabilize the modulation frequency f_(m), and the modulation frequency f_(m) is used as the output of the oscillator to thereby enhance the frequency stability of the oscillator. Therefore, the AC Stark effect caused by the fundamental wave F degrades the detection accuracy of the first sideband wave W1 and the second sideband wave W2 to thereby degrade the stability of the modulation frequency f_(m). Therefore, it degrades the frequency stability of the oscillator.

FIG. 3 is a diagram showing a frequency spectrum of the second light L2 emitted from the wavelength selection section 20.

The second light L2 is light with the fundamental wave F eliminated or decreased in intensity compared to the first light L1. In the example shown in FIG. 3, the second light L2 only has the first sideband wave W1 having the frequency f₁ in the upper sideband with respect to the center frequency f₀, and the second sideband wave W2 having the frequency f₂ in the lower sideband with respect to the center frequency f₀. As described above, in the optical module 2, it is possible to decrease the intensity of the fundamental wave F or to eliminate the fundamental wave F using the wavelength selection section 20.

Hereinafter, a more specific configuration of the atomic oscillator according to the present embodiment will be explained.

FIG. 4 is a block diagram showing a configuration of the atomic oscillator 1.

As shown in FIG. 4, the atomic oscillator 1 includes the optical module 2, a current drive circuit 150, and a modulation circuit 160.

The optical module 2 includes a semiconductor laser 110, a wavelength selection device 120, the gas cell 130, and a light detector 140.

The semiconductor laser 110 generates the first light L1 including the fundamental wave F having the predetermined center wavelength, and first and second sideband waves W1, W2 having respective wavelengths different from each other. The laser beam (the first light L1) emitted from the semiconductor laser 110 is controlled in the center frequency f₀ (the center wavelength λ₀) by the drive current output by the current drive circuit 150, and is then modulated by the output signal (the modulation signal) of the modulation circuit 160. In other words, by superimposing an alternating current having a frequency component of the modulation signal with the drive current by the current drive circuit 150, the first light L1 emitted by the semiconductor laser 110 can be modulated. Thus, the first sideband wave W1 and the second sideband wave W2 are generated in the first light L1. The light generated in the semiconductor laser 110 has a coherent property, and is therefore suitable for obtaining the quantum interference effect.

As shown in FIG. 2B, the first light L1 includes the fundamental wave F having the center frequency f₀ (=ν/λ₀: ν denotes the speed of light; and λ₀ denotes the center wavelength of the first light L1), the first sideband wave W1 having the frequency f₁ in the upper sideband with respect to the center frequency f₀, and the second sideband wave W2 having the frequency f₂ in the lower sideband with respect to the center frequency f₀. The frequency f₁ of the first sideband wave W1 is obtained as f₁=f₀+f_(m), and the frequency f₂ of the second sideband wave W2 is obtained as f₂=f₀−f_(m).

The wavelength selection device 120 selects the first and second sideband waves W1, W2 from the first light L1, and then emits it as the second light L2. The wavelength selection device 120 has the FBG 120 a for selectively emitting light in a predetermined wavelength range, and a temperature control device 120 b for controlling the temperature of the FBG 120 a.

The FBG 120 a is capable of selectively emitting the first sideband wave W1 and the second sideband wave W2 from the first light L1. Thus, it is possible to decrease the intensity of the fundamental wave F of the first light L1 having entered the FBG 120 a or to eliminate the fundamental wave F thereof, and then emit it as the second light L2. In other words, in the second light L2, the intensity of the fundamental wave F is decreased or the fundamental wave F is eliminated compared to the first light L1. In the example shown in FIG. 3, the second light L2 only has the first sideband wave W1 and the second sideband wave W2.

The temperature control device 120 b is capable of varying the wavelength range (the wavelength selection characteristics) of the light to be selected by the FBG 120 a using the thermooptic effect. Here, the thermooptic effect denotes the phenomenon that the refractive index of a material with respect to the light is varied by externally applying heat. Specifically, the temperature control device 120 b controls the temperature of the FBG 120 a to thereby vary the refractive index of the FBG 120 a, and thus control the wavelength selection characteristics of the FBG 120 a. The wavelength selection device 120 is capable of correcting the shift of the wavelength selection characteristics of the FBG 120 a due to the manufacturing error, the environmental variation (e.g., the heat and the light), and so on using the temperature control device 120 b, and is therefore capable of accurately selecting the first sideband wave W1 and the second sideband wave W2 from the first light L1, and then emitting them.

It is also possible for the temperature control device 120 b to adjust the temperature of the FBG 120 a based on the output signal of the light detector 140 to thereby control the wavelength selection characteristics of the FBG 120 a. In the optical module 2, the temperature of the FBG 120 a is adjusted by a feedback loop passing through, for example, the FBG 120 a, the gas cell 130, the light detector 140, and the temperature control device 120 b, and thus the wavelength selection characteristics of the FBG 120 a is controlled.

Further, it is also possible for the temperature control device 120 b to adjust the temperature of the FBG 120 a based on the data of the shift of the wavelength selection characteristics of the FBG 120 a obtained in advance, and then correct the shift of the wavelength selection characteristics of the FBG 120 a.

The gas cell 130 includes gaseous alkali metal atoms (e.g., sodium (Na) atoms, rubidium (Rb) atoms, and cesium (Cs) atoms) encapsulated in a container. The gas cell 130 is irradiated with the second light L2 emitted from the wavelength selection device 120.

When the gas cell 130 is irradiated with the two light waves (the first sideband wave W1 and the second sideband wave W2) having different frequency (wavelength) corresponding to the energy difference between the two ground levels of the alkali metal atoms, the alkali metal atoms cause the EIT phenomenon. If, for example, the alkali metal atoms are cesium atoms, the frequency corresponding to the energy difference between the ground level GL1 at the D1 line and the ground level GL2 is 9.19263 . . . GHz, and therefore, the EIT phenomenon occurs in response to the irradiation with the two light waves having the frequency difference of 9.19263 . . . GHz.

The light detector 140 detects the second light L2 having been transmitted through the gas cell 130, and then outputs a signal having a signal level corresponding to the amount of the light detected. The output signal of the light detector 140 is input to the current drive circuit 150 and the modulation circuit 160. Further, it is also possible for the output signal of the light detector 140 to be input to the temperature control device 120 b. The light detector 140 is, for example, a photo diode.

The current drive circuit 150 generates the drive current having a level corresponding to the output signal of the light detector 140, and then supplies the semiconductor laser 110 with the drive current to thereby control the center frequency f₀ (the center wavelength λ₀) of the first light L1. The center frequency f₀ (the center wavelength λ₀) of the first light L1 is finely adjusted and stabilized by the feedback loop passing through the semiconductor laser 110, the wavelength selection device 120, the gas cell 130, the light detector 140, and the current drive circuit 150.

The modulation circuit 160 generates a modulation signal having the modulation frequency f_(m) corresponding to the output signal of the light detector 140. The modulation signal is supplied to the semiconductor laser 110 while the modulation frequency f_(m) thereof is finely adjusted so that the output signal of the light detector 140 becomes enlarged. The laser beam emitted by the semiconductor laser 110 is modulated in accordance with the modulation signal to thereby generate the first sideband wave W1 and the second sideband wave W2.

It should be noted that the semiconductor laser 110, the wavelength selection device 120, the gas cell 130, and the light detector 140 correspond respectively to the light source 10, the wavelength selection section 20, the gas cell 30, and the light detection section 40 shown in FIG. 1. Further, the FBG 120 a corresponds to the FBG 20 a shown in FIG. 1, and the temperature control device 120 b corresponds to the temperature control section 20 b shown in FIG. 1. Still further, the current drive circuit 150 and the modulation circuit 160 correspond to the control section 50 shown in FIG. 1.

In the atomic oscillator 1 having such a configuration, since the alkali metal atoms fails to cause the EIT phenomenon unless the frequency difference between the first sideband wave W1 and the second sideband wave W2 of the first light L1 generated by the semiconductor laser 110 accurately coincides with the frequency corresponding to the energy difference between the two ground levels of the alkali metal atoms included in the gas cell 130, the detection amount of the light detector 140 varies (increases) in an extremely susceptible manner in accordance with the frequencies of the first sideband wave W1 and the second sideband wave W2. Therefore, feedback control is performed by the feedback loop passing through the semiconductor laser 110, the wavelength selection device 120, the gas cell 130, the light detector 140, and the modulation circuit 160 so that the frequency difference between the first sideband wave W1 and the second sideband wave W2 coincides with the frequency corresponding to the energy difference between the two ground levels of the alkali metal atoms with great accuracy. As a result, since the modulation frequency becomes an extremely stable frequency, the modulation signal can be used as the output signal (clock output) of the atomic oscillator 1.

FIG. 5 is a perspective view schematically showing part (the semiconductor laser 110 and the wavelength selection device 120) of the optical module 2.

As the semiconductor laser 110, a surface emitting laser, for example, can be used. Since the surface emitting laser requires a small current for generating the gain compared to the edge emitting laser, reduction in power consumption can be achieved. It should be noted that it is also possible to use the edge emitting laser as the semiconductor laser 110. As shown in FIG. 5, the first light L1 emitted from the semiconductor laser 110 is collected by an optical element 170, and then enters the FBG 120 a. In the example shown in the drawing, the optical element 170 is a lens for collecting the light L1 emitted from the semiconductor laser 110 to thereby make it enter the FBG 120 a.

The FBG 120 a is formed by providing a periodical variation in the refractive index to the core of an optical fiber. Therefore, the periodical refractive index modulation can be obtained in the longitudinal direction of the optical fiber, and the light signal (the fundamental wave F) within the wavelength range coincident with the period is reflected while the light signals (the first sideband wave W1 and the second sideband wave W2) in another wavelength range are transmitted therethrough without sensing the periodical refractive index variation. In other words, in the FBG 120 a, the reflectance with respect to the first sideband wave W1 and the second sideband wave W2 is low, and the reflectance with respect to the fundamental wave F is high. Therefore, the FBG 120 a is capable of reflecting the fundamental wave F and transmitting the first sideband wave W1 and the second sideband wave W2. Since the optical fiber is used as the FBG 120 a, the FBG 120 a can easily be deformed, and the design freedom can be enhanced. The FBG 120 a can be wound around a bobbin (not shown), for example.

As shown in FIG. 5, the FBG 120 a is disposed above the heating element 122 of the temperature control device 120 b. It should be noted that the positional relationship between the FBG 120 a and the heating element 122 of the temperature control device 120 b is not particularly limited, and it is only required for them to be disposed so that the heat generated by the heating element 122 is conducted to the FBG 120 a. The FBG 120 a is capable of selectively transmitting the first sideband wave W1 and the second sideband wave W2 from the first light L1 having entered.

The temperature control device 120 b has the heating element 122 for supplying the FBG 120 a with heat. When the temperature of the FBG 120 a is varied due to the heat supplied from the temperature control device 120 b, the thermooptic effect occurs to thereby vary the refractive index of the FBG 120 a, and thus the wavelength selection characteristics (the wavelength range of the light to be selected by the FBG) of the FBG 120 a are varied. The heating element 122 is, for example, a resistive element having a predetermined resistance value, and generating heat due to the current flowing therethrough. The temperature control device 120 b can control the temperature of the FBG 120 a by controlling the current amount flowing through the heating element (the resistive element) 122 to thereby adjust the temperature of the heating element 122. It should be noted that the temperature control device 120 b is not particularly limited providing it can control the temperature of the FBG 120 a, and a known hot plate and so on can also be adopted.

The optical module 2 and the atomic oscillator 1 have the following features, for example.

According to the optical module 2, it is possible for the wavelength selection section 120 to decrease the intensity of the fundamental wave F or to eliminate the fundamental wave F. Thus, it is possible to control or prevent the alkali metal atom from being irradiated with the fundamental wave F making no contribution to the EIT phenomenon. Therefore, it is possible to reduce the frequency variation due to the AC Stark effect to thereby provide an oscillator with high frequency stability.

According to the optical module 2, since the wavelength selection device 120 has the temperature control device 120 b for varying the wavelength range of the light to be selected by the FBG 120 a, the shift of the wavelength selection characteristics (the wavelength range of the light to be selected by the FBG) of the FBG 120 a due to manufacturing error or environmental variation (e.g., the heat and the light) can be corrected. Therefore, the wavelength selection device 120 is capable of accurately selecting the first sideband wave W1 and the second sideband wave W2 from the first light L1, and then emitting them.

The wavelength selection characteristics of the FBG 120 a depend on the periodical variation in the refractive index provided to the core of the optical fiber. It is difficult to provide periodical variation in the refractive index to the core of the optical fiber with accuracy in the manufacturing process of the FBG 120 a, and therefore, there is a case in which the manufacturing error is caused in the FBG 120 a. Since the wavelength selection device 120 has the temperature control device 120 b, even in such a case, the wavelength selection device 120 can correct the shift in the wavelength selection characteristics due to the manufacturing error.

In the optical module 2, the temperature control device 120 b is capable of varying the wavelength selection characteristics of the FBG 120 a using the thermooptic effect. Thus, the wavelength selection characteristics of the FBG 120 a can easily be controlled. Further, the temperature control device 120 b is configured including a heating element (a resistive element). Therefore, the wavelength selection device 120 can be made to have a simple configuration.

In the optical module 2, the semiconductor laser 110 can be a surface emitting laser. Since the surface emitting laser requires a small current for generating the gain compared to the edge emitting laser, reduction in power consumption can be achieved.

In the optical module 2, there is provided the optical element 170 for making the light L1 emitted from the semiconductor laser 110 enter the FBG 120 a. Thus, the light L1 generated in the semiconductor laser 110 can efficiently be guided to the FBG 120 a.

In the atomic oscillator 1, there is provided the optical module 2. Therefore, as described above, the frequency stability can be enhanced.

As described above, although the embodiments of the invention are hereinabove explained in detail, it should be understood by those skilled in the art that various modifications not substantially departing from the novel matters and the advantages of the invention are possible. Therefore, such modified examples are included in the scope of the invention.

The entire disclosure of Japanese Patent Application No. 2011-055434, filed Mar. 14, 2011 is expressly incorporated by reference herein. 

1. An optical module for an atomic oscillator using a quantum interference effect, comprising: a light source adapted to emit light including a fundamental wave having a predetermined wavelength, and sideband waves of the fundamental wave; a wavelength selection section receiving the light from the light source, and adapted to transmit the sideband waves out of the light input; a gas cell encapsulating an alkali metal gas, and irradiated with light transmitted through the wavelength selection section; and a light detection section adapted to detect an intensity of light transmitted through the gas cell, wherein the wavelength selection section includes: a fiber Bragg grating, and a temperature control section adapted to control temperature of the fiber Bragg grating.
 2. The optical module for an atomic oscillator according to claim 1, wherein, the temperature control section includes a resistive element presenting a predetermined resistance value, and controls the temperature of the fiber Bragg grating by controlling a current to be applied to the resistive element.
 3. The optical module for an atomic oscillator according to claim 1, wherein, the light source is a surface emitting laser.
 4. The optical module for an atomic oscillator according to claim 1, further comprising: an optical element adapted to make the light emitted from the light source enter the fiber Bragg grating.
 5. An atomic oscillator comprising: the optical module for an atomic oscillator according to claim
 1. 6. An atomic oscillator comprising: the optical module for an atomic oscillator according to claim
 2. 7. An atomic oscillator comprising: the optical module for an atomic oscillator according to claim
 3. 8. An atomic oscillator comprising: the optical module for an atomic oscillator according to claim
 4. 9. An atomic oscillator using a quantum interference effect, comprising: a light source adapted to emit light including a fundamental wave having a predetermined wavelength, and sideband waves of the fundamental wave; a wavelength selection section receiving the light from the light source, and adapted to transmit the sideband waves out of the light input; a gas cell encapsulating an alkali metal gas, and irradiated with light transmitted through the wavelength selection section; and a light detection section adapted to detect an intensity of a light transmitted through the gas cell, wherein the wavelength selection section includes: a fiber Bragg grating, and a temperature control section adapted to control temperature of the fiber Bragg grating. 